{"title":"低成本锁相放大器的漂移","authors":"A. Edgar","doi":"10.1088/0022-3735/22/8/003","DOIUrl":null,"url":null,"abstract":"The limitation on the performance of a lock-in amplifier imposed by noise and drift in the DC amplifier is discussed. Measurements on a commercial instrument show that if the time constant tau is increased whilst holding the ratio of tau to the scan time T fixed, the output noise first falls as tau -0.5, as expected for white noise, but then rises as tau 0.09. This shows that there is an optimal setting for the time constant beyond which the signal-to-noise ratio deteriorates, and suggests that the power density of the drift and noise from the DC amplifier in this instrument has an f-1.18 spectrum. The effect of both drift and noise may be reduced by signal averaging; if the number of scans n is varied while holding both the total measurement time nT and tau /T constant, the averaged RMS noise at first decreases as roughly 1/n, but not 1/n12/, before reaching a limiting value set by white noise. Replacing the first stage DC amplifier with an equivalent circuit based on a low-drift commutating auto-zero instrumentation amplifier reduces the drift and noise by up to a factor of four, and thus extends the useful range of time constants for single-scan measurements.","PeriodicalId":16791,"journal":{"name":"Journal of Physics E: Scientific Instruments","volume":"64 1","pages":"551-553"},"PeriodicalIF":0.0000,"publicationDate":"1989-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Drift in low-cost lock-in amplifiers\",\"authors\":\"A. Edgar\",\"doi\":\"10.1088/0022-3735/22/8/003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The limitation on the performance of a lock-in amplifier imposed by noise and drift in the DC amplifier is discussed. Measurements on a commercial instrument show that if the time constant tau is increased whilst holding the ratio of tau to the scan time T fixed, the output noise first falls as tau -0.5, as expected for white noise, but then rises as tau 0.09. This shows that there is an optimal setting for the time constant beyond which the signal-to-noise ratio deteriorates, and suggests that the power density of the drift and noise from the DC amplifier in this instrument has an f-1.18 spectrum. The effect of both drift and noise may be reduced by signal averaging; if the number of scans n is varied while holding both the total measurement time nT and tau /T constant, the averaged RMS noise at first decreases as roughly 1/n, but not 1/n12/, before reaching a limiting value set by white noise. Replacing the first stage DC amplifier with an equivalent circuit based on a low-drift commutating auto-zero instrumentation amplifier reduces the drift and noise by up to a factor of four, and thus extends the useful range of time constants for single-scan measurements.\",\"PeriodicalId\":16791,\"journal\":{\"name\":\"Journal of Physics E: Scientific Instruments\",\"volume\":\"64 1\",\"pages\":\"551-553\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1989-08-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics E: Scientific Instruments\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1088/0022-3735/22/8/003\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics E: Scientific Instruments","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1088/0022-3735/22/8/003","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The limitation on the performance of a lock-in amplifier imposed by noise and drift in the DC amplifier is discussed. Measurements on a commercial instrument show that if the time constant tau is increased whilst holding the ratio of tau to the scan time T fixed, the output noise first falls as tau -0.5, as expected for white noise, but then rises as tau 0.09. This shows that there is an optimal setting for the time constant beyond which the signal-to-noise ratio deteriorates, and suggests that the power density of the drift and noise from the DC amplifier in this instrument has an f-1.18 spectrum. The effect of both drift and noise may be reduced by signal averaging; if the number of scans n is varied while holding both the total measurement time nT and tau /T constant, the averaged RMS noise at first decreases as roughly 1/n, but not 1/n12/, before reaching a limiting value set by white noise. Replacing the first stage DC amplifier with an equivalent circuit based on a low-drift commutating auto-zero instrumentation amplifier reduces the drift and noise by up to a factor of four, and thus extends the useful range of time constants for single-scan measurements.